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S-Matrix of Nonlocal Scalar Quantum Field Theory in Basis Functions Representation

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S-Matrix of Nonlocal Scalar Quantum Field Theory in Basis Functions Representation Article S-Matrix of Nonlocal Scalar Quantum Field Theory in Basis Functions Representation Ivan V. Chebotarev 1, Vladislav A. Guskov 1, Stanislav L. Ogarkov 1,2,* and Matthew Bernard 1,* 1 Moscow Institute of Physics and Technology (MIPT), Institutskiy Pereulok 9, 141701 Dolgoprudny, Russia; [email protected] (I.V.C.); [email protected] (V.A.G.) 2 Dukhov Research Institute of Automatics (VNIIA), Sushchevskaya 22, 127055 Moscow, Russia * Correspondence: [email protected] (S.L.O.); [email protected] (M.B.) Received: 18 December 2018; Accepted: 12 February 2019; Published: 19 February 2019 Abstract: Nonlocal quantum theory of a one-component scalar field in D-dimensional Euclidean spacetime is studied in representations of S-matrix theory for both polynomial and nonpolynomial interaction Lagrangians. The theory is formulated on coupling constant g in the form of an infrared smooth function of argument x for space without boundary. Nonlocality is given by the evolution of a Gaussian propagator for the local free theory with ultraviolet form factors depending on ultraviolet length parameter l. By representation of the S-matrix in terms of abstract functional integral over a primary scalar field, the S form of a grand canonical partition function is found. By expression of S-matrix in terms of the partition function, representation for S in terms of basis functions is obtained. Derivations are given for a discrete case where basis functions are Hermite functions, and for a continuous case where basis functions are trigonometric functions. The obtained expressions for the S-matrix are investigated within the framework of variational principle based on Jensen inequality. Through the latter, the majorant of S (more precisely, of − ln S) is constructed. Equations with separable kernels satisfied by variational function q are found and solved, yielding results for both polynomial theory j4 (with suggestions for j6) and nonpolynomial sine-Gordon theory. A new definition of the S-matrix is proposed to solve additional divergences which arise in application of Jensen inequality for the continuous case. Analytical results are obtained and numerically illustrated, with plots of variational functions q and corresponding majorants for the S-matrices of the theory. For simplicity of numerical calculation, the D = 1 case is considered, and propagator for free theory G is in the form of Gaussian function typically in the Virton–Quark model, although the obtained analytical inferences are not, in principle, limited to these particular choices. Formulation for nonlocal QFT in momentum k space of extra dimensions with subsequent compactification into physical spacetime is discussed, alongside the compactification process. Keywords: quantum field theory (QFT); scalar QFT; nonlocal QFT; nonpolynomial QFT; Euclidean QFT; S-matrix; form factor; generating functional; abstract functional integral; Gaussian measure; grand canonical partition function; basis functions representation; renormalization group; compactification process 1. Introduction The timeline of Quantum Field Theory (QFT) offers events that are quite asymmetric to each other. Brilliant triumphs, on the one hand, in explanations and predictions of different processes at low-energy Quantum Electrodynamics (QED), high-energy Quantum Chromodynamics (QCD), Theory of Critical Phenomena, and several other branches of the modern science; but catastrophe, on the other hand, in various attempts to describe high-energy physics in scalar theory and QED levels as well as low-energy QCD physics. Identically, in discoveries of renormalizable field theories, Particles 2019, 2, 103–139; doi:10.3390/particles2010009 www.mdpi.com/journal/particles Particles 2019, 2 104 the conjecture that only those make sense is opposing to conjecture that there are any and all theories. Nonetheless, robust indeterminacy is fueled by nonspeculative mathematical theory. In non-Abelian Gauge QFT, unifying electromagnetic and weak interactions into a general model, weak interaction processes are consistently described. In another triumph of non-Abelian QFT, the Standard Model (SM), high-energy problem of QED vanishes in chromodynamic reaction channels, because QCD consistently in a high-energy region has the quintessential property of asymptotic freedom. Recently, the discovery of the Higgs boson, the last SM element in the energy domain, where existence is most natural, occurred. Notably, by the remarkable event confirming validity of SM, a quantum-trivial local scalar field quantum theory is, after all, not quantum-trivial if the SM is a sector of a non-Abelian gauge theory; this is analogous to a QED event. Supersymmetric non-Abelian QFTs as well as Integrable QFTs [1–9] in earnest search for gravity quantum theory and naturally complement superstring theory. Under such sophistication for superstring theory, which is almost surely the strongest pick for the fundamental theory of nature, the ultimate truth, it is not impossible to view all QFTs as effective (low-energy) theory given by renormalizable and nonrenormalizable QFTs, respectively. In other words, every field theory is a limit in superstring theory. Hypothetically, bosonic strings are given consideration if tachyon degrees of freedom form a condensate that is consistently separable by physical expressions; if a perfect factorization, not known to date, is found [10,11]. QFT, symmetrical and fundamental, is nevertheless consistent in the framework; superstring theory is field theory. A Euclidean nonlocal QFT with nonpolynomial interaction Lagrangian is robust theory, mathematically rigorous and logically closed [12–18], dual to statistical physics models, encouraging, among other things, further study [19–25] by a statistical physics analogy that in the reverse direction, informs every structure of nonlocality form factors. Under a robust QFT, the existence of nonlocality, be it fundamental or a phenomenon, in the special case of interest of a four-dimensional spacetime, is undeniable by all uncertainties. The question of how analytical continuation in the Minkowski spacetime is arranged is, however, open due to the lack of existence of the no-go theorem [13,14]. At the auspicious moment, nonlocal QFT is really a self-consistent theory to ensure whether observed processes can or cannot be explained. The nonlocal form factor introduced from physical point of view accounts for meaningful physical processes at too small distances, but is an oversight of experiment design. A QFT problem is considered solved if the mathematical apparatus is created for calculus of the S-matrix of the theory, which is the set of all probability amplitudes of possible transitions between the physical system states under consideration. In hadronic interaction (light hadrons) low-energy physics, nonlocal QFT is called nonlocal quark theory; the Virton–Quark model [14,26–30] is considered effective theory for describing quark confinement field due to no additional field, typically a gluon field, required to ensure quark confinement. With first-principle QCD, it is impossible to obtain satisfactory description of low-energy hadronic interactions. Studies use the robust, original hypothesis that quarks do not exist as arbitrary physical particles, but exist only in a virtual quasiparticle state. The Virton field, in the QFT framework, satisfies two conditions: the free state field is identically zero, and the causal Green function, the field propagator, is nonzero. That is, nonobservability (or nonexistence) simply means identical zero free Virtons field; a free Virton does not exist, and Virtons only exist in a virtual state. In the framework of a functional integral, there is nontrivial generating, functional for the theory, in particular for S-matrix of the theory. Further generalizations of nonlocal QFT, and nonlocal quark theory in particular, include the interaction of electromagnetic field with Virtons. Moreover, nonlocal QFT also arises in a functional (nonperturbative, exact) renormalization group (FRG) [31–34]. Ultraviolet form factors are functions of differential operators (in coordinate representation) and they correspond to FRG regulators, which are the regulators of the FRG flow of different generating functionals in QFT and statistical physics. Particles 2019, 2 105 While FRG regulators are not always chosen for entire analytic functions, they are the most preferred for equations of FRG flow with the best analytical properties. Fundamental contributions to formation and development of nonlocal QFT were made, thanks to Gariy Vladimirovich Efimov, in his earlier papers devoted to local QFT with nonpolynomial interaction Lagrangians [13,35,36], and later papers devoted to nonlocal QFT [12,37–39]. His earlier study was developed in parallel but independently in papers of Efim Samoylovich Fradkin [40–42]; hence, the Efimov–Fradkin Theory, which today in its own right is a subject of study by several authors [43–53]. Furthermore, alternatives of the nonlocality were studied by several authors [54–60]. The idea of nonlocality also was developed in a series of papers by J.W. Moffat and co-authors in the early 90s [61–65], as well as in the 2010s [66–68], in particular, in the context of quantum gravity. Since the study of nonlocal theories is motivated, in particular, by attempts to construct the quantum theory of gravity and QFT in curved spacetime, let us briefly discuss papers of J.W. Moffat [66,68] and possible generalizations. In these papers, a modification of the interaction action
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